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NSR database version of May 2, 2024.

Search: Author = U.Scheib

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1985FU08      Phys.Rev. C32, 418 (1985)

K.Fuchs, W.Eyrich, A.Hofmann, B.Muhldorfer, U.Scheib, H.Schlosser, H.Rebel

Neutron Decay of the Isoscalar Giant Resonance Region in ⁹⁰Zr

NUCLEAR REACTIONS ⁹⁰Zr(α, α'n), E=104 MeV; measured σ(Eα'), σ(θα, θn). ⁹⁰Zr deduced isoscalar giant resonances, multipolarity, decay characteristics.

doi: 10.1103/PhysRevC.32.418
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1984EY01      Phys.Rev. C29, 418 (1984)

W.Eyrich, K.Fuchs, A.Hofmann, U.Scheib, H.Steuer, H.Rebel

Direct Decay Component of the Giant-Monopole-Resonance Region in ²⁰⁸Pb

NUCLEAR REACTIONS ²⁰⁸Pb(α, α'n), E=104 MeV; measured σ(Eα'), σ(θα, θn); deduced preequilibrium neutron decay. ²⁰⁸Pb deduced giant monopole resonance decay characteristics.

doi: 10.1103/PhysRevC.29.418
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1983OR01      Phys.Rev. C27, 1988 (1983)

H.Ortner, W.Eyrich, A.Hofmann, U.Scheib

Separation of Direct and Compound Nuclear Contributions in Inelastic α Scattering

NUCLEAR REACTIONS ²⁸Si(α, α'γ), E=10, 16.5 MeV; measured σ(θ), αγ(θ); deduced direct, compound nuclear contributions. DWBA, Hauser-Feshbach analyses.

doi: 10.1103/PhysRevC.27.1988
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1983VO08      Phys.Rev. C28, 1925 (1983)

F.Vogler, J.Bottcher, W.Eyrich, A.Hofmann, M.Meyer, U.Scheib

Deuteron-Gamma Angular Correlations in the Reactions ^24,26Mg, ^28,30Si(d, d₁γ) at E(d) = 10 MeV

NUCLEAR REACTIONS ^24,26Mg, ^28,30Si(d, d'γ), E=10 MeV; measured σ(θ), dγ(θ); deduced optical model parameter restrictions, reaction mechanism. ^24,26Mg, ^28,30Si deduced shape. Coupled-channels, DWBA analyses. Enriched targets.

doi: 10.1103/PhysRevC.28.1925
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0725.

1981EY02      Phys.Rev. C24, 2720 (1981)

W.Eyrich, H.Hassold, A.Hofmann, B.Muhldorfer, U.Scheib, H.Rebel

Search for E0 Strength in the Giant Resonance Region of ¹²C

NUCLEAR REACTIONS ¹²C(α, α'), E=104 MeV; measured σ(Eα), σ(θ). ¹²C deduced no monopole resonance.

doi: 10.1103/PhysRevC.24.2720
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1981ST25      Phys.Rev.Lett. 47, 1702 (1981)

H.Steuer, W.Eyrich, A.Hofmann, H.Ortner, U.Scheib, R.Stamminger, D.Steuer, H.Rebel

Neutron Decay of the Giant Quadrupole Resonance Region in ²⁰⁸Pb

NUCLEAR REACTIONS ²⁰⁸Pb(α, α'n), E=104 MeV; measured nα-coin, Eα, En. ²⁰⁸Pb deduced GQR branching ratio. ²⁰⁷Pb levels deduced populating γ-multipolarity.

doi: 10.1103/PhysRevLett.47.1702
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1979EY02      Phys.Rev.Lett. 43, 1369 (1979)

W.Eyrich, A.Hofmann, U.Scheib, S.Schneider, F.Vogler, H.Rebel

Decay of the Isoscalar Giant Resonances in ²⁰⁸Pb

NUCLEAR REACTIONS ²⁰⁸Pb(α, α'), E=104 MeV; measured α'γ(θ). ²⁰⁸Pb deduced T=0, GQR, fine structure following n decay.

doi: 10.1103/PhysRevLett.43.1369
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1979RO09      Phys.Lett. 88B, 51 (1979)

H.Rost, W.Eyrich, A.Hofmann, U.Scheib, F.Vogler, H.Rebel

A Study of the Giant Resonance Region of ⁴⁰Ca by Inelastic Scattering Of 104 MeV α-Particles

NUCLEAR REACTIONS ⁴⁰Ca(α, α'), E=104 MeV; measured σ(θ). ⁴⁰Ca resonances deduced L, β₂, energy-weighted sum rule strengths for E2. DWBA analysis.

doi: 10.1016/0370-2693(79)90111-4
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1979SC05      Phys.Lett. 80B, 180 (1979)

S.Schneider, W.Eyrich, A.Hofmann, U.Scheib, F.Vogler

The Influence of Deformations of the Optical Potential on Analyzing Power and p₁-γ Angular Correlation in the Reaction ¹¹⁴Cd(p, p')

NUCLEAR REACTIONS ¹¹⁴Cd(p, p'), E=11 MeV; measured σ(θ), A(θ), pγ(θ); deduced influence of β, spin-orbit β in optical potential. Coupled-channels analysis.

doi: 10.1016/0370-2693(79)90192-8
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1979SC15      Phys.Rev. C20, 71 (1979)

S.Schneider, W.Eyrich, A.Hofmann, U.Scheib, F.Vogler

Reaction ¹¹⁴Cd(p, p') by Use of Polarized Protons and Proton-γ Angular Correlations

NUCLEAR REACTIONS ¹¹⁴Cd(p, p'), (p, p'γ), (polarized p, p'), (polarized p, p'γ), E=11 MeV; measured σ(θ), A(θ), pγ(θ), spin flip probability. ¹¹⁴Cd deduced evidence against oblate deformation for harmonic vibrator model. Coupled-channel analysis. Enriched target.

doi: 10.1103/PhysRevC.20.71
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1978DR05      Nucl.Phys. A301, 205 (1978)

W.Draxler, W.Eyrich, A.Hofmann, U.Scheib, F.Vogler

Evidence for Detour Transitions in Internal Bremsstrahlung of ⁹⁰Y

RADIOACTIVITY ⁹⁰Sr, ⁹⁰Y; measured γ CP (internal bremsstrahlung). ⁹⁰Y deduced evidence for detour transitions. ⁹⁰Sr+⁹⁰Y source.

doi: 10.1016/0375-9474(78)90261-0
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1978EY02      Fizika, Suppl. 10, 45 (1978)

W.Eyrich, A.Hofmann, U.Scheib, S.Schneider, F.Vogler, H.Rebel

The Deformation of ²⁶Mg from Particle-Gamma Angular Correlations

NUCLEAR REACTIONS ^24,26Mg, ²⁸Si(α, α'), E=104 MeV; measured αγ(θ). ^24,26Mg, ²⁸Si level deduced β. Coupled-channels analysis.

1978HO25      Nuovo Cim. 53A, 396 (1978)

P.Holleczek, A.Hofmann, U.Scheib, F.Vogler

Deuteron Break-up Model Analyses of Cross-Section, Analysing Power and Angular Correlation of the Reactions ⁵²Cr(d, p) and ⁵⁸Ni(d, p)

NUCLEAR REACTIONS ⁵²Cr, ⁵⁸Ni(d, p), E=10 MeV; ⁵²Cr, ⁵⁸Ni(p, p), E=5.45 MeV; calculated σ(θ), vector analyzing power, pγ(θ). Johnson-Soper adiabatic model.

1977EY03      Nucl.Phys. A287, 119 (1977)

W.Eyrich, A.Hofmann, U.Scheib, S.Schneider, F.Vogler, H.Rebel

Alpha-Gamma Angular Correlations in the Reaction ²⁴Mg(α, α₁γ) at E = 104 MeV

NUCLEAR REACTIONS ²⁴Mg(α, α'γ), E=104 MeV; measured in-plane α'γ(θ). ²⁴Mg deduced sign of the quadrupole deformation parameter. Coupled channels analyses, enriched target.

doi: 10.1016/0375-9474(77)90567-X
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1977SC12      Lett.Nuovo Cim. 18, 301 (1977)

U.Scheib, A.Hofmann, F.Vogler

The (d, d₁) Vector Analysing Power of the Reaction ²⁴Mg(d, d₁) and the d₁-γ Angular Correlation

NUCLEAR REACTIONS ²⁴Mg(polarized d, d'), E=10 MeV; measured A(θ).

doi: 10.1007/BF02784849
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1976EY02      Phys.Lett. 63B, 406 (1976)

W.Eyrich, A.Hofmann, U.Scheib, S.Schneider, F.Vogler, H.Rebel

Alpha-Gamma Angular Correlation Measurements as a Sensitive Method Determining the Sign of the Nuclear Quadrupole Deformation

NUCLEAR REACTIONS ²⁴Mg(α, α'γ), E=104 MeV; measured γγ(θ). ²⁴Mg levels deduced sign of β₂.

doi: 10.1016/0370-2693(76)90381-6
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1976EY03      Nucl.Instrum.Methods 138, 543 (1976)

W.Eyrich, A.Hofmann, U.Scheib, S.Schneider, F.Vogler

Measurement and Evaluation of Particle-γ Angular Correlations for the Study of Nuclear Reaction Mechanisms

NUCLEAR REACTIONS ⁵²Cr(d, pγ); measured pγ-coin. ²⁴Mg(d, d'γ); measured d'γ-coin.

doi: 10.1016/0029-554X(76)90321-9
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1975SC12      Phys.Rev.Lett. 34, 1586 (1975)

U.Scheib, A.Hofmann, F.Vogler

d-γ Angular Correlations as a Test for the Importance of Multistep Processes in the Reaction ²⁴Mg(d, d')

NUCLEAR REACTIONS ²⁴Mg(d, d'γ), E=10 MeV; measured d'γ(θ), σ(Ed', θ); deduced optical, deformation parameters.

doi: 10.1103/PhysRevLett.34.1586
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1974EY03      Phys.Rev. C10, 2512 (1974)

W.Eyrich, S.Schneider, A.Hofmann, U.Scheib, F.Vogler

Proton-γ Angular Correlations in the Reaction ⁵²Cr(d, pγ)⁵³Cr

NUCLEAR REACTIONS ⁵²Cr(d, pγ), E=10 MeV; measured σ(Ep, Eγ, θ), pγ-coin. ⁵³Cr transitions deduced L.

doi: 10.1103/PhysRevC.10.2512
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1973SC05      Nucl.Phys. A203, 177 (1973)

U.Scheib, A.Hofmann, G.Philipp, F.Vogler

The Effect of the Potential Parameters on the Spectroscopic Factors of The ²⁴Mg(d, p)²⁵Mg Reaction

NUCLEAR REACTIONS ²⁴Mg(d, p), E=10 MeV; measured σ(Ep, θ). ²⁵Mg levels deduced S, dependence on potential parameters. Enriched target.

doi: 10.1016/0375-9474(73)90431-4
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