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NSR database version of May 24, 2024.

Search: Author = C.Blasing

Found 8 matches.

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1990DE20      Nucl.Phys. A513, 29 (1990)

A.Degener, C.Blasing, R.D.Heil, A.Jung, U.Kneissl, H.H.Pitz, H.Schacht, S.Schennach, R.Stock, C.Wesselborg

Dipole Excitations in 48Ti Studied by Nuclear Resonance Fluorescence

NUCLEAR REACTIONS 48Ti(γ, γ'), E=4.1-14 MeV bremsstrahlung; measured Eγ, Iγ, γ(θ), azimuthal asymmetries. 48Ti deduced levels, J, π, Γ0, reduced transition probabilities. Enriched target, partially polarized, unpolarized beam, nuclear resonance fluorescence experiment.

doi: 10.1016/0375-9474(90)90340-R
Citations: PlumX Metrics


1986RA01      Phys.Rev.Lett. 56, 568 (1986)

R.Ratzek, U.E.P.Berg, C.Blasing, A.Jung, S.Schennach, R.Stock, F.-J.Urban, H.Wickert

Electric and Magnetic Dipole Transitions to Bound States in 206Pb

NUCLEAR REACTIONS 206Pb(polarized γ, γ'), E=7 MeV bremsstrahlung; measured Iγ(θ), asymmetry. 206Pb deduced levels, J, π, γ-multipolarity, B(λ).

doi: 10.1103/PhysRevLett.56.568
Citations: PlumX Metrics


1986WI08      Phys.Rev. C34, 835 (1986)

H.Wickert, K.Ackermann, K.Bangert, U.E.P.Berg, C.Blasing, W.Naatz, A.Ruckelshausen, S.Schennach, R.Stock

Parities of Bound Dipole States in 40Ar

NUCLEAR REACTIONS 40Ar(polarized γ, γ), E=17 MeV bremsstrahlung; measured Eγ, asymmetry(θ=90°). 40Ar deduced levels, J, π, γ-multipolarity, B(λ). Nuclear resonance fluorescence technique.

doi: 10.1103/PhysRevC.34.835
Citations: PlumX Metrics


1984BE26      Phys.Lett. 140B, 191 (1984)

U.E.P.Berg, K.Ackermann, K.Bangert, C.Blasing, W.Naatz, R.Stock, K.Wienhard, M.K.Brussel, T.E.Chapuran, B.H.Wildenthal

Bound State M1 Transitions in sd-Shell Nuclei

NUCLEAR REACTIONS 20,22Ne, 24Mg, 28,30Si, 32,34S(γ, γ'), E=65 MeV bremsstrahlung; 26Mg(γ, γ'), E not given; measured Eγ, Iγ. 22Ne, 26Mg, 28,30Si, 32,34S(polarized γ, γ), E=22 MeV bremsstrahlung; measured γ asymmetry, polarization effect. 20,22Ne, 24,26Mg, 28,30Si, 32,34S levels deduced B(M1), (Γ0/Γ), Γ0. Nuclear resonance fluorescence technique, linearly polarized γ-beam. Shell model comparison.

doi: 10.1016/0370-2693(84)90918-3
Citations: PlumX Metrics


1984BE54      Phys.Lett. 149B, 59 (1984)

U.E.P.Berg, C.Blasing, J.Drexler, R.D.Heil, U.Kneissl, W.Naatz, R.Ratzek, S.Schennach, R.Stock, T.Weber, H.Wickert, B.Fischer, H.Hollick, D.Kollewe

Photoexcitation of Low-Lying Collective States in 156,158,160Gd

NUCLEAR REACTIONS 156,158,160Gd(γ, γ'), E=2.8-3.4 MeV bremsstrahlung; measured Eγ, Iγ. 156,158,160Gd levels deduced Γγ, B(M1), transition collectivity.

doi: 10.1016/0370-2693(84)91551-X
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1982WI06      Phys.Rev.Lett. 49, 18 (1982)

K.Wienhard, K.Ackermann, K.Bangert, U.E.P.Berg, C.Blasing, W.Naatz, A.Ruckelshausen, D.Ruck, R.K.M.Schneider, R.Stock

Parity of Bound Dipole States in 208Pb

NUCLEAR REACTIONS 208Pb(polarized γ, γ), E=10 MeV bremsstrahlung; measured Eγ, Iγ, asymmetry. 208Pb deduced level, J, π, B(M1), Γ02/Γ. Linearly polarized beam.

doi: 10.1103/PhysRevLett.49.18
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1981BE32      Phys.Lett. 103B, 301 (1981)

U.E.P.Berg, D.Ruck, K.Ackermann, K.Bangert, C.Blasing, K.Kobras, W.Naatz, R.K.M.Schneider, R.Stock, K.Wienhard

Parities of Dipole Ground-State Transitions in 52Cr

NUCLEAR REACTIONS 52Cr(polarized γ, γ), E=7-9 MeV bremsstrahlung; measured Eγ, Iγ, asymmetry. 52Cr deduced strong E1 transitions, B(M1) limit. Nuclear resonance fluorescence technique.

doi: 10.1016/0370-2693(81)90228-8
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1981WI12      Z.Phys. A302, 185 (1981)

K.Wienhard, C.Blasing, K.Ackermann, K.Bangert, U.E.P.Berg, K.Kobras, W.Naatz, D.Ruck, R.K.M.Schneider, R.Stock

Parities of Strong Dipole Ground State Transitions in 88Sr

NUCLEAR REACTIONS 88Sr(polarized γ, γ), E=16 MeV bremsstrahlung; measured asymmetry. 88Sr levels deduced π. Nuclear resonance fluorescence technique, enriched targets.

doi: 10.1007/BF01413049
Citations: PlumX Metrics


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