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NSR database version of May 2, 2024.

Search: Author = U.Zurmuhl

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1991SC13      Nucl.Phys. A528, 189 (1991)

K.P.Schelhaas, J.M.Henneberg, N.Wieloch-Laufenberg, U.Zurmuhl, B.Ziegler, M.Schumacher, F.Wolf

Nuclear Photon Scattering by Si

NUCLEAR REACTIONS ²⁸Si(γ, γ), (γ, γ'), E=15-140 MeV; measured σ(E, θ). ²⁸Si deduced E1, E2 resonance parameters, radius parameters.

doi: 10.1016/0375-9474(91)90423-4
Citations: PlumX Metrics

1990SC02      Nucl.Phys. A506, 307 (1990)

K.P.Schelhaas, J.M.Henneberg, N.Wieloch-Laufenberg, U.Zurmuhl, B.Ziegler, M.Schumacher, F.Wolf

Nuclear Photon Scattering by ¹²C

NUCLEAR REACTIONS ¹²C(γ, γ), (γ, γ'), E=15-140 MeV; measured σ(E, θ). ¹²C deduced E1, E2 resonance parameters, radius parameters, polarizability of bound nucleons.

doi: 10.1016/0375-9474(90)90389-4
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0876.

1988SC16      Nucl.Phys. A489, 189 (1988)

K.P.Schelhaas, J.M.Henneberg, M.Sanzone-Arenhovel, N.Wieloch-Laufenberg, U.Zurmuhl, B.Ziegler, M.Schumacher, F.Wolf

Nuclear Photon Scattering by ²⁰⁸Pb

NUCLEAR REACTIONS ²⁰⁸Pb(γ, γ'), E=10-100 MeV; measured σ(θ) vs E. ²⁰⁸Pb deduced giant resonance parameters. Monochromatic beam.

doi: 10.1016/0375-9474(88)90149-2
Citations: PlumX Metrics

1985SC10      Nucl.Phys. A438, 493 (1985)

M.Schumacher, U.Zurmuhl, F.Smend, R.Nolte

Low-Energy Electric-Dipole Transition Widths Predicted by the Giant Dipole Resonance and Statistical Models

NUCLEAR STRUCTURE A=6-20; A=21-44; calculated electric transition hindrance factors. GDR, statistical models.

doi: 10.1016/0375-9474(85)90388-4
Citations: PlumX Metrics

1983RU03      Phys.Rev. C27, 559 (1983)

P.Rullhusen, U.Zurmuhl, F.Smend, M.Schumacher, H.G.Borner, S.A.Kerr

Giant Dipole Resonances and Coulomb Correction Effect in Delbruck Scattering Studied by Elastic and Raman Scattering of 8.5 to 11.4 MeV Photons

NUCLEAR REACTIONS ²³⁸U, ²³²Th, ²⁰⁹Bi(γ, γ), (γ, γ'), E=8.5-11.4 MeV; measured σ(θ) for elastic, Raman scattering; deduced Delbruck scattering Coulomb correction. ²³⁸U, ²³²Th, ²⁰⁹Bi deduced GDR parameters.

doi: 10.1103/PhysRevC.27.559
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0413.

1983ZU04      Z.Phys. A314, 171 (1983)

U.Zurmuhl, P.Rullhusen, F.Smend, M.Schumacher, H.G.Borner, S.A.Kerr

Nuclear Resonance Scattering Studies on ²³⁸U using a Dense Series of γ-Ray Photons

NUCLEAR REACTIONS ²³⁸U(γ, γ), (γ, γ'), E=4-7 MeV; measured Eγ, Iγ, σ(θγ). ²³⁸U deduced GDR, nonstatistical resonance strengths, Γ. Photon beam from ¹⁸¹Ta, ¹⁴¹Pr(n, γ), nuclear resonance fluorescence.

1982RU03      Nucl.Phys. A382, 79 (1982)

P.Rullhusen, U.Zurmuhl, W.Muckenheim, F.Smend, M.Schumacher, H.G.Borner

Coulomb Correction Effect in Delbruck Scattering and Nuclear Resonance Fluorescence of 2 to 10 MeV Photons on ²³⁸U

NUCLEAR REACTIONS ²³⁸U(γ, γ), (γ, γ'), E=2.75-9.72 MeV; measured Eγ, Iγ, σ(θ), elastic scattering, nuclear resonance fluorescence. ²³⁸U deduced levels, γ-branching.

doi: 10.1016/0375-9474(82)90442-0
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0416.

1982ZU01      Phys.Lett. 114B, 99 (1982)

U.Zurmuhl, P.Rullhusen, F.Smend, M.Schumacher, H.G.Borner

The Distribution of E1 Strength below Particle Threshold Studied by Resonant Scattering of Gamma Rays

NUCLEAR REACTIONS ²³⁸U(γ, γ), E=2.75-6.5 MeV; measured σ(θ), total σ(absorption) vs E; ¹⁸¹Ta(γ, γ), E=3-6.75 MeV; ¹⁶⁵Ho(γ, γ), E=3.5-6.75 MeV; measured total σ(absorption) vs E. ²³⁸U, ¹⁸¹Ta, ¹⁶⁵Ho deduced average γ-branching ratio, E1 transition strength distribution, nonstatistical deviations from GDR Lorentzian. Nuclear resonance fluorescence.

doi: 10.1016/0370-2693(82)90123-X
Citations: PlumX Metrics