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NSR database version of April 29, 2024.

Search: Author = S.Norbert

Found 7 matches.

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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, T_1/2, 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, T_1/2, δ, quadrupole moment, shape coexistence. Weak coupling model.

doi: 10.1007/BF02115850
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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, T_1/2, B(λ), δ, Γp, Γ, intrinsic quadrupole moments. Shell model.

doi: 10.1007/BF01424765
Citations: PlumX Metrics

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, T_1/2, J, π, rotational bands, intrinsic quadrupole moments, K, Nilsson assignments. Collective, shell models.

doi: 10.1007/BF01425158
Citations: PlumX Metrics

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
Citations: PlumX Metrics