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NSR database version of April 29, 2024.

Search: Author = H.Schobbert

Found 9 matches.

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1983GE09      J.Phys.(London) G9, 939 (1983)

H.U.Gersch, H.Schobbert, D.Wohlfarth

Search for a Three-Particle Component of the E(cm) = 11.1 MeV 5- Resonance in the 12C + 16O Reaction

NUCLEAR REACTIONS 12C(16O, α), E=25-27 MeV; measured σ(E). 12C(16O, α12C), E=25.964 MeV; measured σ(E(12C)), (12C)(12C)-coin. 28Si deduced resonance, no direct three-body decay.

doi: 10.1088/0305-4616/9/8/016
Citations: PlumX Metrics


1983KL03      Nucl.Phys. A398, 476 (1983)

P.Kleinwachter, H.U.Gersch, H.Schobbert

Investigation of Isobaric Analog Resonances in 53Mn

NUCLEAR REACTIONS 52Cr(p, p'γ), (p, γ), E=2.72-2.82 MeV; measured σ(E). 52Cr(p, p), (p, p'), (p, p'γ), (p, γ), E=4.06-4.12, 4.57-4.62, 4.65-4.71 MeV; measured σ(E, θ). 53Mn deduced IAR, S(p), S(p'), Γγ. 53Cr, 53Mn deduced analog pair Coulomb displacement energies. Enriched targets.

doi: 10.1016/0375-9474(83)90297-X
Citations: PlumX Metrics


1981SC05      J.Phys.(London) G7, L73 (1981)

H.Schobbert, H.U.Gersch, H.J.Wiebicke

On the Three-Body Decay of the E(CM)=19.7 MeV 14+ Resonance in 16O + 12C-Induced Reactions

NUCLEAR REACTIONS 12C(16O, α), E(cm)=19.7 MeV; analyzed (12C)(12C)-coin data. 28Si resonance deduced symmetric three-body decay.

doi: 10.1088/0305-4616/7/4/006
Citations: PlumX Metrics


1979FO12      J.Phys.(London) G5, 1267 (1979)

I.Fodor, J.Sziklai, P.Kleinwachter, H.Schobbert, F.Herrmann

Fragmented g9/2 Isobaric Analogue Resonances in the 52Cr(p, γ)53Mn Reaction

NUCLEAR REACTIONS 52Cr(p, γ), E=4.080-4.320 MeV; measured Eγ, Iγ, Iγ(θ). 53Mn deduced g9/2, IAR, Γγ0. Enriched target.

doi: 10.1088/0305-4616/5/9/011
Citations: PlumX Metrics


1979FO19      J.Phys.(London) G5, 1267 (1979)

I.Fodor, J.Sziklai, P.Kleinwachter, H.Schobbert, F.Herrmann

Fragmented g9/2 Isobaric Analogue Resonances in the 52Cr(p, γ)53Mn Reaction

NUCLEAR REACTIONS 52Cr(p, γ), E=4080-4320 keV; measured Eγ, Iγ, Iγ(θ). 53Mn deduced g9/2 IAS, Γγ, spreading width. Enriched target.

doi: 10.1088/0305-4616/5/9/011
Citations: PlumX Metrics


1978BE32      Izv.Akad.Nauk SSSR, Ser.Fiz. 42, 60 (1978); Bull.Acad.Sci.USSR, Phys.Ser. 42, No.1, 48 (1978)

K.Beckert, H.-U.Gersch, F.Herrmann, D.Hinke, P.Kleinvechter, H.Muller, H.Schobbert, I.Fodor, I.Szentpetery

Time Structure of the 2d5/2 Analog State of 59Cu

NUCLEAR REACTIONS 58Ni(p, p), (p, γ), (p, p'γ), E=4.7-5.2 MeV; measured σ(E, θ). 59Cu deduced analog state fine structure, Γp, S, L.

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0874.


1978FO20      J.Phys.(London) G4, 1117 (1978)

I.Fodor, J.Sziklai, B.Kardon, J.Rama Rao, K.Beckert, F.Herrmann, H.Schobbert

g9/2 Isobaric Analogue Resonances in the 56Fe(p, γ)57Co Reaction

NUCLEAR REACTIONS 56Fe(p, γ), E=3660-3850 keV; measured Eγ, Iγ, γ(θ). 57Co deduced IAS, Γγ, J, π, B(λ).

doi: 10.1088/0305-4616/4/7/016
Citations: PlumX Metrics


1974BE72      Izv.Akad.Nauk SSSR, Ser.Fiz. 38, 2083 (1974); Bull.Acad.Sci.USSR, Phys.Ser. 38, No.10, 60 (1974)

K.Beckert, H.U.Gersch, F.Herrmann, P.Kleinvechter, H.Schobbert, I.Fodor, I.Szentpetery

The d5/2 Analog Resonance Excited in 58Ni(p, γ)59Cu

NUCLEAR REACTIONS 58Ni(p, γ), E=4.7-5.2 MeV; measured σ(E;Eγ, θ). 58Ni(p, p), E=4.7-5.2 MeV; measured σ(E, θ). 59Cu deduced isobar analog resonances, J, π, level-width.

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF1162.


1974BE73      Izv.Akad.Nauk SSSR, Ser.Fiz. 38, 2087 (1974); Bull.Acad.Sci.USSR, Phys.Ser. 38, No.10, 63 (1974)

K.Beckert, H.U.Gersch, D.Grambole, F.Herrmann, P.Kleinvechter, C.Schneiderait, H.Schobbert, H.J.Thomas

The g9/2 Isobaric Analog Resonance in 53Mn

NUCLEAR REACTIONS 52Cr(p, γ), E=3.9-4.6 MeV; measured σ(E;Eγ, θ). 52Cr(p, p'γ), E=3.9-4.6 MeV; measured σ(E;Eγ). 53Mn deduced isobar analog resonances, γ-branching.


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