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NSR database version of April 26, 2024.

Search: Author = A.Hofmann

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1996BA58      Phys.Rev. C54, 1877 (1996)

P.D.Barnes, G.Diebold, G.Franklin, B.Quinn, R.Schumacher, J.Seydoux, V.Zeps, P.Birien, W.Dutty, H.Fischer, J.Franz, E.Rossle, H.Schledermann, H.Schmitt, R.Todenhagen, W.Breunlich, N.Nagele, R.Broders, R.von Frankenberg, K.Kilian, W.Oelert, K.Rohrich, K.Sachs, T.Sefzick, G.Sehl, M.Ziolkowski, R.A.Eisenstein, D.Hertzog, R.Tayloe, H.Dennert, W.Eyrich, R.Geyer, J.Hauffe, A.Hofmann, M.Kirsch, R.A.Kraft, F.Stinzing, N.Hamann, T.Johansson, S.Ohlsson

Observables in High-Statistics Measurements of the Reaction (p-bar)p → (Λ-bar)Λ

NUCLEAR REACTIONS 1H(p-bar, X), E at 1.642, 1.918 GeV/c; measured Λ(Λ-bar) production associated σ(θ), polarizations, spin correlations, analyzing powers, singlet fractions; deduced CP, CPT violation phenomena upper limits.

doi: 10.1103/PhysRevC.54.1877
Citations: PlumX Metrics


1994BA70      Phys.Lett. 331B, 203 (1994)

P.D.Barnes, P.Birien, W.H.Breunlich, W.Dutty, R.A.Eisenstein, G.Ericsson, W.Eyrich, H.Fischer, R.von Frankenberg, G.Franklin, J.Franz, R.Geyer, N.Hamann, D.Hertzog, A.Hofmann, T.Johansson, K.Kilian, M.Kirsch, R.-A.Kraft, W.Oelert, S.Ohlsson, B.Quinn, K.Rohrich, E.Rossle, H.Schledermann, H.Schmitt, T.Sefzick, G.Sehl, J.Seydoux, F.Stinzing, R.Tayloe, R.Todenhagen, V.Zeps, M.Ziolkowski

Study of the Reaction (p-bar)p → (Lambda-bar)Lambda Below 6 MeV Excess Energy

NUCLEAR REACTIONS 1H(p-bar, X), E=low; measured σ(E) vs excess energy, σ(θ) for ((lambda-bar)-lambda) production.

doi: 10.1016/0370-2693(94)90964-4
Citations: PlumX Metrics


1993MU13      Phys.Rev. C48, 981 (1993)

R.Muller, R.Baran, U.Bohnert, P.Helbig, G.Herrmann, A.Hofmann, O.Jakel, H.Kruger, D.Malz, W.Menzel, H.-W.Ortner, L.Schweinzer, S.Wirth

ππ-Angular Correlations for π-p → π+π-n in the Region of the Δ Dominance

NUCLEAR REACTIONS 1H(π-, π+π-), E=284 MeV; measured σ(θ(π+), θ(π-)) vs E(π+), invariant mass distribution; deduced reaction mechanism. Weinberg's Lagrangian based models, relativistic corrections, contribution of nonlinear terms.

doi: 10.1103/PhysRevC.48.981
Citations: PlumX Metrics


1992RI05      Phys.Rev.Lett. 69, 1504 (1992)

S.Riess, G.Enders, A.Hofmann, W.Kuhn, V.Metag, R.Novotny, W.Mittig, Y.Schutz, A.C.C.Villari, H.Emling, H.Grein, E.Grosse, W.Henning, R.Holzmann, R.Kulessa, T.Matulewicz, H.J.Wollersheim

Measurement of the Impact Parameter in Intermediate Energy Heavy Ion Collisions

NUCLEAR REACTIONS 158Gd(40Ar, X), E=44 MeV/nucleon; measured fragment charge distribution, γ(fragment)-coin, γ-multiplicity; deduced hard photon multiplicity impact parameter dependence.

doi: 10.1103/PhysRevLett.69.1504
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1991BA19      Nucl.Phys. A526, 575 (1991)

P.D.Barnes, G.Diebold, G.Franklin, C.Maher, B.Quinn, J.Seydoux, K.Kilian, R.Besold, W.Eyrich, R.von Frankenberg, A.Hofmann, D.Malz, F.Stinzing, P.Woldt, P.Birien, W.Dutty, J.Franz, N.Hamann, E.Rossle, H.Schledermann, H.Schmitt, H.-J.Urban, R.A.Eisenstein, D.Hertzog, W.Oelert, G.Sehl, B.E.Bonner, G.Ericsson, T.Johansson, S.Ohlsson, W.H.Breunlich, P.Pawlek

Study of the Reaction (p-bar)p → (Lambda-bar)Lambda at 1.546 and 1.695 GeV/c

NUCLEAR REACTIONS 1H(p-bar, X), E at 1.546, 1.695 GeV/c; measured hyperon-antihyperon exclusive production σ, σ(θ), polarization, spin correlation.

doi: 10.1016/0375-9474(91)90434-8
Citations: PlumX Metrics


1990OR03      Phys.Rev.Lett. 64, 2759 (1990)

H.-W.Ortner, R.Baran, U.Bohnert, M.Dillig, G.Herrmann, A.Hofmann, P.Helbig, O.Jakel, W.Kluge, H.Kruger, D.Malz, H.Matthay, R.Muller, W.Menzel, L.Schweinzer, S.Wirth

Kinematically Complete Measurement of the Reaction π-p → π+π-n in the Region of Δ Dominance as a Test of Chiral Lagrangians

NUCLEAR REACTIONS 1H(π-, π-π+), E=247-330 MeV; measured π+π-(θ); deduced σ(θ(π+), σ(π-)) vs π+ momentum. Kinematically complete experiment.

doi: 10.1103/PhysRevLett.64.2759
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1989GI01      Nucl.Instrum.Methods Phys.Res. A276, 169 (1989)

H.J.Gils, H.Jelitto, H.Schlosser, S.Zagromski, J.Buschmann, W.Eyrich, A.Hofmann, J.Kiener, A.Lehmann, H.Rebel

The QQDS Magnetic Spectrograph ' Little John ' at the Karlsruhe Cyclotron II. Experimental procedures and performance

NUCLEAR REACTIONS 12C(6Li, 6Li), E=158 MeV; measured 6Li spectra. 208Pb, 12C(6Li, αX), E=156 MeV; measured σ(θα, Eα). 12C(6Li, 6Li'), E=156 MeV; measured σ(θ), σ(θ(6Li), E(6Li)). 12C(6Li, 6He), E=156 MeV; measured σ(θ(6He), E(6He)).

doi: 10.1016/0168-9002(89)90629-3
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1530.


1988BA27      Phys.Rev. C37, 2892 (1988)

R.Baran, J.Gotz, A.Hofmann, D.Malz, R.Muller, R.Olszewski, H.W.Ortner, D.Dehnhard

Excitation Function of the 15.11 MeV (1+, T=1) State in 12C from (π, π'γ) Angular Correlations

NUCLEAR REACTIONS 12C(π, π'γ), E=116, 140, 162, 180, 226 MeV; measured σ(E(π)), πγ-coin. 12C levels deduced relative σ(ratio) vs E.

doi: 10.1103/PhysRevC.37.2892
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1988OL02      Phys.Rev. C37, 2665 (1988)

R.Olszewski, R.Baran, A.Hofmann, S.Krell, H.W.Ortner, J.Orzechowsky, G.Schmidtlein, F.Vogler, W.List, G.R.Smith, D.Dehnhard, M.Thies

Medium Effects in (π, π'γ) Angular Correlations on 12C(2+)

NUCLEAR REACTIONS 12C(π, π'γ), E=116, 140, 162, 180, 226 MeV; measured π(γ)-coin, πγ(θ). Isobar-hole model.

doi: 10.1103/PhysRevC.37.2665
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1987EY01      Phys.Rev. C36, 416 (1987)

W.Eyrich, A.Hofmann, A.Lehmann, B.Muhldorfer, H.Schlosser, H.Wirth, H.J.Gils, H.Rebel, S.Zagromski

E0 Strength in 12C from 6Li Scattering

NUCLEAR REACTIONS 12C(6Li, 6Li'), E=156 MeV; measured σ(E(6Li), θ), θ=0°-2.5°. 12C deduced E0 transition strength distribution, EWSR fraction. DWBA analysis.

doi: 10.1103/PhysRevC.36.416
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1987KR06      Nucl.Instrum.Methods Phys.Res. A255, 531 (1987)

S.Krell, A.Hofmann, R.Olszewski, H.W.Ortner, F.Vogler

Determination of the Efficiency of Gamma Detectors from Particle-Gamma Angular Correlations

NUCLEAR REACTIONS 12C(α, α'γ), E=11 MeV; measured αγ(θ, φ); deduced detector efficiency.

doi: 10.1016/0168-9002(87)91223-X
Citations: PlumX Metrics


1986HO08      Z.Phys. B62, 335 (1986)

A.Hofmann, A.Willmeroth, R.Vianden

Lattice Defects in Rhodium and Iridium Trapped at 111In Probe Atoms

RADIOACTIVITY 111In(EC); measured γγ(θ, H, t) in Ir single crystal; deduced lattice defects in fcc metals.


1986OL07      Phys.Rev.Lett. 57, 2143 (1986)

R.Olszewski, R.Baran, A.Hofmann, S.Krell, H.W.Ortner, J.Orzechowski, G.Schmidtlein, F.Vogler, G.R.Smith, W.List, D.Dehnhard, M.Thies

Test of the Δ-Hole Model through the Energy Dependence of (π, π'γ) Angular Correlations on 12C

NUCLEAR REACTIONS 12C(π, π'γ), E=116, 140, 162, 180, 226 MeV; measured πγ(θ), πγ(φ); deduced isobar-nucleus dynamics role. NaI detectors. Isobar-hole model.

doi: 10.1103/PhysRevLett.57.2143
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1985DE53      Phys.Lett. 111A, 208 (1985)

S.H.Devare, A.Hofmann, J.Kotthaus, R.Vianden

Selective Site Occupancy of 117Cd in Beryllium

RADIOACTIVITY 117Cd(β-); measured γγ(θ, H, t); deduced two different quadrupole interaction frequencies. Source selective site occupancy in Be.

doi: 10.1016/0375-9601(85)90578-X
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1981ST11      Nucl.Phys. A363, 301 (1981)

J.Stumm, A.Hofmann

Multishell Coupled-Channels Analysis of Inelastic Deuteron Scattering on (s, d) Shell Nuclei at E(d)= 10 MeV

NUCLEAR REACTIONS 24,26Mg, 28,30Si(polarized d, d), (polarized d, d'), E=10 MeV; analyzed σ(θ), dγ(θ), analyzing power vs θ. Multishell, coupled-channels method.

doi: 10.1016/0375-9474(81)90258-X
Citations: PlumX Metrics


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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1980ST19      J.Phys.(London) G6, 875 (1980)

J.Stumm, A.Hofmann

A Microscopic Multishell-Coupled-Channels Description of Inelastic Deuteron Scattering on 58Ni at Ed = 10 MeV

NUCLEAR REACTIONS 58Ni(d, d'), E=10 MeV; measured σ(θ), dγ(θ). Multishell form factors, coupled channels calculation.

doi: 10.1088/0305-4616/6/7/010
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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.


1978ST18      J.Phys.(London) G4, L229 (1978)

J.Stumm, A.Hofmann

Multishell-Model Description of Low-Energy Proton Scattering

NUCLEAR REACTIONS 58Ni(polarized p, p), (polarized p, p'), E=20.4, 30.3 MeV; calculated σ(θ), A(θ).

doi: 10.1088/0305-4616/4/9/003
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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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1975EY01      Phys.Rev. C11, 1658 (1975)

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

Gamma-Decay Data from Particle-γ Correlation Functions at Fixed γ Angles

NUCLEAR REACTIONS 52Cr(d, pγ), E=10 MeV; measured σ(Ep, θ), pγ(θ). 53Cr levels deduced γ-mixing.

doi: 10.1103/PhysRevC.11.1658
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1975PR08      Nucl.Phys. A255, 64 (1975)

R.Prasad, A.Hofmann, F.Vogler

Investigation of Backward α-Particle Scattering in 24Mg and 28Si Through α-γ Angular Correlations

NUCLEAR REACTIONS 24Mg(α, α'γ), E=15.5-17.0 MeV; 28Si(α, α'γ), E=15.0-16.2 MeV; measured reaction plane double-differential cross sections; Hauser-Feshbach analyses of angular correlations. Enriched targets.

doi: 10.1016/0375-9474(75)90147-5
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0630.


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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1974KU18      Z.Phys. 271, 49 (1974)

E.Kuhlmann, A.Hofmann, W.Albrecht

High Spin States in 21Ne

NUCLEAR REACTIONS 18O(α, nγ), E=9-10.5 MeV; measured nγ-coin, σ(E, Eγ, θ), nγ(θ). 21Ne levels deduced K, J, π, γ-branching ratios.

doi: 10.1007/BF01676400
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1974PR12      Phys.Rev. C10, 1577 (1974)

R.Prasad, A.Hofmann, F.Vogler

Study of the Reaction 26Mg(p, αγ)23Na Through α-γ Angular Correlations

NUCLEAR REACTIONS 26Mg(p, αγ), E=9.5, 9.75, 10.0, 10.25 MeV; measured σ(E, Eα, θ), αγ(θ). Hauser-Feshbach analysis, enriched target.

doi: 10.1103/PhysRevC.10.1577
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1974VO01      Phys.Rev. C9, 242 (1974)

F.Vogler, M.Berg, A.Hofmann, H.Wagner

Proton-γ Angular Correlations in the Reaction 24Mg(d, pγ)25Mg

NUCLEAR REACTIONS 24Mg(d, pγ), E=10 MeV; measured σ(Ep, Eγ, θ), pγ(θ). 25Mg deduced transitions.

doi: 10.1103/PhysRevC.9.242
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1974WU01      Z.Phys. 269, 365 (1974)

W.Wuhr, A.Hofmann, G.Philipp

Optical Model and DWBA Analysis of the α-Particle Scattering for the Nuclei 26Mg and 28,30Si Including Hauser-Feshbach Contributions

NUCLEAR REACTIONS 26Mg, 28,30Si(α, α), (α, α'), E=15-16.4 MeV; measured σ(E, θ), σ(E, Eα', θ). 26Mg, 28,30Si levels deduced β2, spin cut-off parameters.

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0617.


1973KU15      Nucl.Phys. A213, 82 (1973)

E.Kuhlmann, W.Albrecht, A.Hofmann

The γ-Ray Decay of Levels in 30S

NUCLEAR REACTIONS 28Si(3He, n), E=7.0-10.0 MeV; measured n-γ(θ), Doppler-shift attenuation. 30S deduced levels, T1/2, J, γ-branchings. Natural, enriched targets.

doi: 10.1016/0375-9474(73)90183-8
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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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1973SC12      Z.Phys. 260, 35 (1973)

B.Schneck, A.Hofmann

Systematische Untersuchungen zum Optischen Modell der Deuteronenstreuung an 24,26Mg und 28,30Si

NUCLEAR REACTIONS 24,26Mg, 28,30Si(d, d), E=10 MeV; measured σ(θ). Deduced optical model parameters.

doi: 10.1007/BF01398068
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1973WA32      Phys.Lett. 47B, 497 (1973)

H.Wagner, A.Hofmann, F.Vogler

Determination and DWBA Analyses of Transition Matrix Elements in the Reaction 26Mg(α, α'γ)26Mg

NUCLEAR REACTIONS 26Mg(α, α'), E=15 MeV; measured σ(θ).

doi: 10.1016/0370-2693(73)90025-7
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1972BE78      Phys.Lett. 42B, 211 (1972)

M.Berg, A.Hofmann, K.Thomas, H.Rebel, G.W.Schweimer

Coupled-Channels Analysis of Deuteron Scattering from 30Si at E = 10 MeV

NUCLEAR REACTIONS 30Si(d, d), (d, d'), E=10 MeV; measured σ(θ). 30Si deduced deformation parameter β2.

doi: 10.1016/0370-2693(72)90063-9
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1972HE35      Nucl.Instrum.Methods 105, 91 (1972)

G.Hempel, A.Hofmann, K.Kilian

Analysing Powers for Protons Elastically Scattered by a Thick Silicon Target

NUCLEAR REACTIONS Si(p, p), E < 6 MeV; measured analyzing power(E;θ).

doi: 10.1016/0029-554X(72)90497-1
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1971HO31      Lett.Nuovo Cim. 2, 133 (1971)

A.Hofmann, F.Vogler

An Examination of Coupled-Channel Calculations for the Reaction 24Mg(d, p)25Mg

NUCLEAR REACTIONS 24Mg(d, p), E=10 MeV; measured σ(θ). Coupled channel analysis.

doi: 10.1007/BF02772736
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1971KR03      Z.Phys. 242, 308 (1971)

G.Kroner, A.Hofmann, G.Philipp, K.Thomas

Beitrage von direkten und Compoundprozessen zur Reaktion 40Ca(d, α)38K bei E = 5 - 10 MeV

NUCLEAR REACTIONS 40Ca(d, α), E=5-10 MeV; measured σ(E;Eα, θ); deduced compound-nucleus contribution.

doi: 10.1007/BF01396980
Citations: PlumX Metrics


1971PH01      Nucl.Phys. A160, 654 (1971)

G.Philipp, W.-D.Emmerich, A.Hofmann, G.Kroner, K.Thomas

The Collective Nature of the Low-Lying States in 27Al and 23Na Investigated with (p, α) Reactions

NUCLEAR REACTIONS 26Mg, 30Si(p, α), E=10.0-11.5 MeV; 27Al(p, α), E=6.8-8.2, 10.0-11.5 MeV; 31P(p, α), E=5.8-7.3, 10.0-11.5 MeV; measured σ(E, Eα, θ); deduced reaction mechanism. Enriched 26Mg, 30Si targets.

doi: 10.1016/0375-9474(71)90107-2
Citations: PlumX Metrics


1970EM01      Z.Phys. 231, 279 (1970)

W.-D.Emmerich, A.Hofmann, G.Philipp

Untersuchung der Niedrigliegenden Anregungszustande in 25Mg und 27Al mit Hilfe der Deuteronenstreuung

NUCLEAR REACTIONS 25Mg, 27Al(d, d), (d, d'), E=10 MeV; measured σ(Ed', θ). 25Mg, 27Al deduced levels, J, π.

doi: 10.1007/BF01401039
Citations: PlumX Metrics


1969HO08      Nucl.Phys. A131, 435 (1969)

A.Hofmann, W.-D.Emmerich, G.Philipp

Einfluss der Kollektivstruktur der Endkern-Zustande Auf (d, α)-Wirkungsquerschnitte in der sd-Schale

NUCLEAR REACTIONS 25Mg, 29Si, 31P(d, α), E=10.1 MeV; 23Na(d, α), E=10.0, 11.0 MeV; measured σ(Eα, θ). 21Ne, 23Na, 27Al, 29Si deduced levels, reaction mechanism. Enriched 25Mg, 29Si targets.

doi: 10.1016/0375-9474(69)90547-8
Citations: PlumX Metrics


1968HO04      Phys.Letters 26B, 378 (1968)

A.Hofmann, W.Emmerich, H.Dinter, G.Philipp

Abhangigkeit des Wirkungsquerschnitts fur 27Al(d, α)25Mg von Den Rotationszustanden des 25Mg

NUCLEAR STRUCTURE 25Mg; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0370-2693(68)90618-7
Citations: PlumX Metrics


1968HO14      Nucl.Phys. A113, 86(1968)

A.Hofmann, W.Emmerich, H.Dinter, G.Philipp

Die Reaktion 27Al(d, α)25Mg

NUCLEAR REACTIONS 27Al(d, α), E=4.74, 9.2, 10.1 MeV; measured σ(E;Eα, θ). 25Mg deduced levels, σ direct, reaction mechanism.

doi: 10.1016/0375-9474(68)90885-3
Citations: PlumX Metrics


1968TH05      Z.Physik 217, 128 (1968)

K.Thomas, A.Hofmann

Der Polarisationsgrad der Neutronen Aus der Reaktion D(d, n)3He fur E = 80 bis 140 keV

NUCLEAR STRUCTURE 2H; measured not abstracted; deduced nuclear properties.

doi: 10.1007/BF01390501
Citations: PlumX Metrics


1964BA51      Helv. Phys. Acta 37, 602 (1964)

R.Balzer, D.Bharucha, F.Heinrich, A.Hofmann

β-Spektrometer mit Trochoidformigen Bahnen

NUCLEAR STRUCTURE 207Bi; measured not abstracted; deduced nuclear properties.


1963BA58      Helv.Phys.Acta 36, 495 (1963)

R.Balzer, D.Bharucha, F.Heinrich, A.Hofmann

Messung der Li-γ-Strahlung mit einem Hochauflosenden Paarspektrometer

NUCLEAR STRUCTURE 7Li; measured not abstracted; deduced nuclear properties.


1963HO08      Z.Phys. 173, 402 (1963)

A.Hofmann

γ-Strahlung bei Inelastischer Streuung von 14 MeV Neutronen an Calcium, Sauerstoff und Kohlenstoff

NUCLEAR STRUCTURE 12C, 16O, 40Ca; measured not abstracted; deduced nuclear properties.

doi: 10.1007/BF01380702
Citations: PlumX Metrics


1958HO95      Helv.Phys.Acta 31, 591 (1958)

A.Hofmann, P.Stoll

Investigation of (γ, pn) and (γ, d) Reactions with Gamma Energies to 32 MeV


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