NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = P.Betz Found 18 matches. 1991HE05 Z.Phys. A338, 23 (1991) F.Heidinger, P.Betz, W.Brendler, F.Glatz, A.Hoffmann, H.Ropke, B.H.Wildenthal The Structure of 25Mg NUCLEAR REACTIONS 24Mg(d, p), E=6.5 MeV; measured σ(Ep). 22Ne(α, nγ), E=11.8-15.5 MeV; measured Eγ, Iγ, nγ-coin, nγ(θ). 25Mg deduced levels, J, π, branching ratio, δ, T1/2, B(λ), T. Shell model.
doi: 10.1007/BF01279113
1989HO07 Z.Phys. A332, 289 (1989) A.Hoffmann, P.Betz, H.Ropke, B.H.Wildenthal Structure of the Mirror Nuclei 21Ne and 21Na NUCLEAR REACTIONS 18O(α, nγ), E=12-15.4 MeV; measured nγ(θ), σ(En), nγ-coin. 18O(α, 2nγ), E=13.4 MeV; measured σ(En). 21Ne deduced levels, J, π, δ. Shell model comparison. NUCLEAR STRUCTURE 21Ne, 21Na; calculated levels, Gamow-Teller matrix elements, T1/2. Shell model.
1983BI08 Z.Phys. A313, 123 (1983) E.Bitterwolf, A.Burkard, P.Betz, F.Glatz, F.Heidinger, Th.Kern, R.Lehmann, S.Norbert, H.Ropke, C.Schneider, J.Siefert Shape Coexistence and Other Aspects of Nuclear Structure in 40Ar NUCLEAR REACTIONS 37Cl(α, pγ), E=12, 13 MeV; measured pγ-coin, γ linear polarization, DSA. 40Ar deduced levels, J, π, γ branching, T1/2, δ, quadrupole moment, shape coexistence. Weak coupling model.
doi: 10.1007/BF02115850
1982BE52 Z.Phys. A309, 163 (1982) P.Betz, E.Bitterwolf, A.Burkard, F.Glatz, F.Heidinger, Th.Kern, R.Lehmann, S.Norbert, H.Ropke, C.Schneider, J.Siefert Spectroscopy of Highly Excited States in 29Si NUCLEAR REACTIONS 28Si(d, pγ), E=6.5, 7 MeV; 26Mg(α, nγ), E=12, 14, 15 MeV; 27Al(3He, pγ), E=9 MeV; measured σ(Ep), σ(En), γp(θ), γp-coin. 29Si deduced levels, J, π, K, deformation, rotational band structure. Shell model.
doi: 10.1007/BF01414978
1981GL01 Phys.Rev.Lett. 46, 1559 (1981) F.Glatz, P.Betz, J.Siefert, F.Heideniger, H.Ropke Excited Kπ = 0+ Rotational Band in 28Si NUCLEAR REACTIONS 25Mg(α, n), E=14.5 MeV; measured nγ(θ); 27Al(p, γ), E=2160, 2312 keV; measured Eγ, Iγ, DSA. 28Si deduced levels, J, π, K, rotational band structure, ground state quadrupole moments, B(λ). Ge(Li) detectors, tof.
doi: 10.1103/PhysRevLett.46.1559
1981GL05 Z.Phys. A303, 239 (1981) F.Glatz, J.Siefert, P.Betz, E.Bitterwolf, A.Burkard, F.Heidinger, Th.Kern, R.Lehmann, S.Norbert, H.Ropke Structure of 28Si from the Spectroscopy of High-Spin States NUCLEAR REACTIONS 25Mg(α, nγ), E=14, 15.5 MeV; measured nγ-coin, nγ(θ), DSA. 27Al(p, γ), E=2.16, 2.312 MeV; measured Eγ, Iγ, DSA. 28Si deduced levels, J, π, rotational bands, T1/2, B(λ), δ, Γp, Γ, intrinsic quadrupole moments. Shell model.
doi: 10.1007/BF01424765
1980BI14 Z.Phys. A298, 279 (1980) E.Bitterwolf, P.Betz, A.Burkard, F.Glatz, F.Heidinger, T.Kern, R.Lehmann, S.Norbert, J.Siefert, H.Ropke Structure of 30Si from the Spectroscopy of Highly Excited States NUCLEAR REACTIONS 27Al(α, pγ), E=12, 14.1, 15 MeV; measured pγ(θ), linearly polarized γp-coin, DSA. 30Si deduced levels, T1/2, J, π, rotational bands, intrinsic quadrupole moments, K, Nilsson assignments. Collective, shell models.
doi: 10.1007/BF01425158
1980KE01 Z.Phys. A294, 51 (1980) T.Kern, P.Betz, E.Bitterwolf, F.Glatz, H.Ropke Density of High-Spin States in 38Ar and 42Ca NUCLEAR REACTIONS 35Cl(α, pγ), E=16 MeV; 39K(α, pγ), E=15.14 MeV; measured pγ-coin. 42Ca, 38Ar deduced levels, π, γ-branching, high J state density. Weak coupling model.
doi: 10.1007/BF01473121
1979GL07 Z.Phys. A293, 57 (1979) F.Glatz, P.Betz, E.Bitterwolf, A.Burkard, F.Heidinger, T.Kern, R.Lehmann, S.Norbert, H.Ropke High-Spin States in 48Ti NUCLEAR REACTIONS 45Sc(α, pγ), E=11, 12, 13 MeV; measured pγ(θ), DSA, Eγ, Iγ, σ(Ep). 48Ti deduced levels, J, π, γ-branching ratio. Shell-model interpretation.
doi: 10.1007/BF01414785
1978GL05 Fizika, Suppl. 10, 9 (1978) High-Spin States in 48Ti NUCLEAR REACTIONS 45Sc(α, pγ), E=11 MeV; measured pγ(θ), DSA. 48Ti deduced high spin states, T1/2, B(λ). Shell model.
1976BE13 Z.Phys. A276, 295 (1976) P.Betz, E.Bitterwolf, B.Busshardt, H.Ropke Deformed States of High Spin in 42Ca NUCLEAR REACTIONS 39K(α, pγ), E=14, 15 MeV; measured pγ(θ), DSA. 42Ca deduced levels, K, J, π, T1/2, quadrupole moment, γ-branching, δ, B(λ).
doi: 10.1007/BF01412107
1976BI15 J.Phys.(London) G2, L171 (1976) Collective Structure of Negative Parity States in 42Ca NUCLEAR REACTIONS 39K(α, pγ), E=14, 15 MeV; measured σ(Ep, Eγ), DSA. 42Ca levels deduced J, π, T1/2, γ-branching, δ.
doi: 10.1088/0305-4616/2/3/009
1976GL10 Z.Phys. A278, 319 (1976) F.Glatz, G.Pappert, A.Brachat, P.Betz, H.Ropke High-Spin States in 38Ar NUCLEAR REACTIONS 35Cl(α, pγ), E=14 MeV; measured Eγ, Iγ, γγ(θ), γ(t). 38Ar deduced levels, J, π, T1/2, δ, γ-branching.
1974BE68 Z.Phys. 271, 195 (1974) P.Betz, H.Ropke, F.Glatz, G.Hammel, V.Glattes, W.Brendler Evidence for the Coexistence of Spherical and Deformed States in 38Ar NUCLEAR REACTIONS 35Cl(α, pγ), E=14, 14.5 MeV; measured pγ(θ), DSA. 38Ar deduced levels, K, J, π, T1/2, E2 strengths.
doi: 10.1007/BF01676390
1974RO10 Z.Phys. 266, 55 (1974) H.Ropke, G.Hammel, W.Brendler, P.Betz, V.Glattes New Aspects of the Rotational Model in 25Mg NUCLEAR REACTIONS 22Ne(α, nγ), E=8.0, 8.8 MeV; 24Mg(d, pγ), E=6 MeV; measured γ(θ), pγ(θ), DSA. 25Mg levels deduced T1/2, J, π, γ-mixing.
1974RO24 Z.Phys. 268, 391 (1974) H.Ropke, P.Betz, G.Bender, V.Glattes, G.Hammel, W.Brendler High-Spin States in 27Al NUCLEAR REACTIONS 26Mg(p, γ), E=2174 keV; measured σ(Eγ, θ). 24Mg(α, pγ), E=13, 15, 15.2 MeV; measured DSA, pγ-coin, pγ(θ), σ(Ep, Eγ). 27Al deduced levels, T1/2, J, π, γ-mixing, γ-width. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0664. 1974RO39 Z.Phys. 271, 59 (1974) H.Ropke, W.Brendler, P.Betz, V.Glattes, G.Hammel Lifetime Measurements in 25Mg NUCLEAR REACTIONS 24Mg(d, pγ), E=6 MeV; measured DSA, pγ-coin. 25Mg levels deduced T1/2, K, J, π, transition rates.
1973BE28 Z.Phys. 261, 351 (1973) Search for High-Spin States in 29Si Using a Neutron Time-of-Flight Spectrometer NUCLEAR REACTIONS 26Mg(α, nγ), E=11, 12, 13, 14 MeV; measured nγ-coin, Eγ, Iγ, DSA. 29Si deduced levels, J, π, T1/2.
doi: 10.1007/BF01399333
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