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NSR database version of May 9, 2024.

Search: Author = G.Finnas

Found 3 matches.

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1980AR02      Nucl.Phys. A334, 71 (1980)

S.E.Arnell, S.Sjoberg, O.Skeppstedt, E.Wallander, A.Nilsson, G.Finnas

High Spin States of ⁸³Sr

NUCLEAR REACTIONS ⁸⁰Kr(α, n), E=16-21 MeV; ⁸²Kr(α, 3n), E=45 MeV; measured Eγ, Iγ(E, θγ), γγ-coin. ⁸³Sr deduced levels, J, π. Enriched targets. Ge(Li) detectors.

doi: 10.1016/0375-9474(80)90140-2
Citations: PlumX Metrics

1978AR19      Z.Phys. A289, 89 (1978)

S.E.Arnell, S.Sjoberg, O.Skeppstedt, E.Wallander, A.Nilsson, Z.P.Sawa, G.Finnas

A Study of ⁸⁷Zr by (α, xn) Reactions

NUCLEAR REACTIONS ⁸⁴Sr(α, nγ), (α, pγ), E=18, 21 MeV; ⁸⁶Sr(α, 3nγ), (α, 2npγ), E=45, 51 MeV; measured Eγ, Iγ, γγ-coin, pγ-coin, DSA. ⁸⁷Zr deduced levels, T_1/2, J, π, δ, B(λ). Compared with core-cluster coupling model. ⁸⁷Y levels deduced γ-branching.

doi: 10.1007/BF01408500
Citations: PlumX Metrics

1977AR04      Nucl.Phys. A280, 72 (1977)

S.E.Arnell, S.Sjoberg, O.Skeppstedt, E.Wallander, A.Nilsson, G.Finnas

High-Spin States of ⁸⁵Sr

NUCLEAR REACTIONS ⁸²Kr(α, n), E=14-21 MeV; ⁸⁴Kr(α, 3n), E=35-45 MeV; measured Eγ, Iγ(Eα, θ(γ)), γγ-coin, Doppler shift attenuation. ⁸⁵Sr deduced levels, J, π, T_1/2, δ. Enriched targets, Ge(Li) detectors.

doi: 10.1016/0375-9474(77)90294-9
Citations: PlumX Metrics