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NSR database version of April 27, 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
Citations: PlumX Metrics

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
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