NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = F.Glatz Found 16 matches. 1997BR07 Z.Phys. A357, 157 (1997) J.Brenneisen, B.Erhardt, F.Glatz, Th.Kern, R.Ott, H.Ropke, J.Schmalzlin, P.Siedle, B.H.Wildenthal The Structure of 32S I. Spectroscopy of the Highly-Excited States NUCLEAR REACTIONS 29Si(α, n), E=14.4 MeV; measured neutron spectra, γn-coin, γn(θ). 31P(p, γ), E=2-3.3 MeV; measured Eγ, Iγ, γ(θ). 32S deduced high-spin levels, J, π, T, γ-branching ratios, T1/2, δ, B(M1). Other data input.
doi: 10.1007/s002180050231
1997BR12 Z.Phys. A357, 377 (1997) J.Brenneisen, B.Erhardt, F.Glatz, Th.Kern, R.Ott, H.Ropke, J.Schmalzlin, P.Siedle, B.H.Wildenthal The Structure of 32S II. Shell Model Interpretation NUCLEAR STRUCTURE 32S; calculated levels, Γγ, branching ratios, other aspects. Shell model.
doi: 10.1007/s002180050257
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
1988LI31 Z.Phys. A331, 409 (1988) M.Lickert, J.Brenneisen, F.Glatz, D.Grathwohl, A.Martinez v.Remisowski, H.Ropke, J.Siefert, B.H.Wildenthal The Structure of 27Al NUCLEAR REACTIONS 24Mg(α, pγ), E=14.2, 15, 15.6 MeV; measured proton spectra, Eγ, Iγ, pγ-coin, pγ(θ). 26Mg(p, γ), E=1.82-2.574 MeV; measured γ(θ). 27Al deduced levels, J, π, δ, γ-branching ratios, B(λ), T1/2. Shell model. NUCLEAR STRUCTURE 27Al; calculated levels, γ-branching ratios, T1/2, B(λ). Shell model.
1986GL05 Z.Phys. A324, 173 (1986) F.Glatz, M.Lickert, A.Burkard, Th.Kern, R.Lehmann, S.Norbert, H.Ropke, J.Siefert, B.H.Wildenthal Search for Missing Predicted High-Spin States in 28Si NUCLEAR REACTIONS 27Al(p, γ), E=1.911, 2.073 keV; measured Eγ, Iγ, γ(θ), linear polarization, DSA. 28Si deduced levels, J, π, T, K, rotational band structure, Γγ. Shell model comparison.
1986GL06 Z.Phys. A324, 187 (1986) F.Glatz, S.Norbert, E.Bitterwolf, A.Burkard, F.Heidinger, Th.Kern, R.Lehmann, H.Ropke, J.Siefert, C.Schneider, B.H.Wildenthal High-Spin States in 26Mg NUCLEAR REACTIONS 23Na(α, pγ), E=14.2, 16 MeV; measured σ(Ep), pγ-coin, pγ(θ), DSA. 26Mg deduced levels, J, π, T1/2, K, γ-branching, δ, B(λ), intrinsic quadrupole moments, rotational band structure, prolate to oblate deformation transition.
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.
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
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